This gives the following values at different velocities:--

+----------+-------+-------+-------+-------+-------+-------+-------+-------+-------+-------+-------+

| v = | 0.3 | 0.5 | 0.7 | 1 | 1½ | 2 | 3 | 5 | 7 | 10 | 15 |

| | | | | | | | | | | | |

| [zeta] = |0.01215|0.01025|0.00944|0.00883|0.00836|0.00812|0.90788|0.00769|0.00761|0.00755|0.00750|

+----------+-------+-------+-------+-------+-------+-------+-------+-------+-------+-------+-------+

In using this value of [zeta] when v is not known, it is best to

proceed by approximation.

§ 98. _Darcy and Bazin's Expression for the Coefficient of

Friction._--Darcy and Bazin's researches have shown that [zeta] varies

very greatly for different degrees of roughness of the channel bed,

and that it also varies with the dimensions of the channel. They give

for [zeta] an empirical expression (similar to that for pipes) of the

form

[zeta] = a(1 + [beta]/m); (6)

where m is the hydraulic mean depth. For different kinds of channels

they give the following values of the coefficient of friction:--

+-------------------------------------------------+--------+------+

| Kind of Channel. | [alpha]|[beta]|

+-------------------------------------------------+--------+------+

| I. Very smooth channels, sides of smooth | | |

| cement or planed timber | .00294 | 0.10 |

| II. Smooth channels, sides of ashlar, brickwork,| | |

| planks | .00373 | 0.23 |

|III. Rough channels, sides of rubble masonry or | | |

| pitched with stone | .00471 | 0.82 |

| IV. Very rough canals in earth | .00549 | 4.10 |

| V. Torrential streams encumbered with detritus | .00785 | 5.74 |

+-------------------------------------------------+--------+------+

The last values (Class V.) are not Darcy and Bazin's, but are taken

from experiments by Ganguillet and Kutter on Swiss streams.

The following table very much facilitates the calculation of the mean

velocity and discharge of channels, when Darcy and Bazin's value of

the coefficient of friction is used. Taking the general formula for

the mean velocity already given in equation (2a) above,

v = c [root](mi),

where c = [root](2g/[zeta]), the following table gives values of c for

channels of different degrees of roughness, and for such values of the

hydraulic mean depths as are likely to occur in practical

calculations:--

Values of c in v = c[root](mi), deduced from Darcy and Bazin's Values.

+----------+-----------+----------+---------+----------+--------------+

| |Very Smooth| Smooth | Rough |Very Rough| Excessively |

| Mean | Channels, | Channels,|Channels,| Channels,|Rough Channels|

|Depth = m.| Cement. |Ashlar or | Rubble |Canals in | encumbered |

| | |Brickwork.| Masonry.| Earth. |with Detritus.|

+----------+-----------+----------+---------+----------+--------------+

| .25 | 125 | 95 | 57 | 26 | 18.5 |

| .5 | 135 | 110 | 72 | 36 | 25.6 |

| .75 | 139 | 116 | 81 | 42 | 30.8 |

| 1.0 | 141 | 119 | 87 | 48 | 34.9 |

| 1.5 | 143 | 122 | 94 | 56 | 41.2 |

| 2.0 | 144 | 124 | 98 | 62 | 46.0 |

| 2.5 | 145 | 126 | 101 | 67 | .. |

| 3.0 | 145 | 126 | 104 | 70 | 53 |

| 3.5 | 146 | 127 | 105 | 73 | .. |

| 4.0 | 146 | 128 | 106 | 76 | 58 |

| 4.5 | 146 | 128 | 107 | 78 | .. |

| 5.0 | 146 | 128 | 108 | 80 | 62 |

| 5.5 | 146 | 129 | 109 | 82 | .. |

| 6.0 | 147 | 129 | 110 | 84 | 65 |

| 6.5 | 147 | 129 | 110 | 85 | .. |

| 7.0 | 147 | 129 | 110 | 86 | 67 |

| 7.5 | 147 | 129 | 111 | 87 | .. |

| 8.0 | 147 | 130 | 111 | 88 | 69 |

| 8.5 | 147 | 130 | 112 | 89 | .. |

| 9.0 | 147 | 130 | 112 | 90 | 71 |

| 9.5 | 147 | 130 | 112 | 90 | .. |

| 10.0 | 147 | 130 | 112 | 91 | 72 |

| 11 | 147 | 130 | 113 | 92 | .. |

| 12 | 147 | 130 | 113 | 93 | 74 |

| 13 | 147 | 130 | 113 | 94 | .. |

| 14 | 147 | 130 | 113 | 95 | .. |

| 15 | 147 | 130 | 114 | 96 | 77 |

| 16 | 147 | 130 | 114 | 97 | .. |

| 17 | 147 | 130 | 114 | 97 | .. |

| 18 | 147 | 130 | 114 | 98 | .. |

| 20 | 147 | 131 | 114 | 98 | 80 |

| 25 | 148 | 131 | 115 | 100 | .. |

| 30 | 148 | 131 | 115 | 102 | 83 |

| 40 | 148 | 131 | 116 | 103 | 85 |

| 50 | 148 | 131 | 116 | 104 | 86 |

| [oo] | 148 | 131 | 117 | 108 | 91 |

+----------+-----------+----------+---------+----------+--------------+

§ 99. _Ganguillet and Kutter's Modified Darcy Formula._--Starting from

the general expression v = c[root]mi, Ganguillet and Kutter examined

the variations of c for a wider variety of cases than those discussed

by Darcy and Bazin. Darcy and Bazin's experiments were confined to

channels of moderate section, and to a limited variation of slope.

Ganguillet and Kutter brought into the discussion two very distinct

and important additional series of results. The gaugings of the

Mississippi by A. A. Humphreys and H. L. Abbot afford data of

discharge for the case of a stream of exceptionally large section and

or very low slope. On the other hand, their own measurements of the

flow in the regulated channels of some Swiss torrents gave data for

cases in which the inclination and roughness of the channels were

exceptionally great. Darcy and Bazin's experiments alone were

conclusive as to the dependence of the coefficient c on the dimensions

of the channel and on its roughness of surface. Plotting values of c

for channels of different inclination appeared to indicate that it

also depended on the slope of the stream. Taking the Mississippi data

only, they found

c = 256 for an inclination of 0.0034 per thousand,

= 154 " " 0.02 "

so that for very low inclinations no constant value of c independent

of the slope would furnish good values of the discharge. In small

rivers, on the other hand, the values of c vary little with the slope.

As regards the influence of roughness of the sides of the channel a

different law holds. For very small channels differences of roughness

have a great influence on the discharge, but for very large channels

different degrees of roughness have but little influence, and for

indefinitely large channels the influence of different degrees of

roughness must be assumed to vanish. The coefficients given by Darcy

and Bazin are different for each of the classes of channels of

different roughness, even when the dimensions of the channel are

infinite. But, as it is much more probable that the influence of the

nature of the sides diminishes indefinitely as the channel is larger,

this must be regarded as a defect in their formula.

Comparing their own measurements in torrential streams in Switzerland

with those of Darcy and Bazin, Ganguillet and Kutter found that the

four classes of coefficients proposed by Darcy and Bazin were

insufficient to cover all cases. Some of the Swiss streams gave

results which showed that the roughness of the bed was markedly

greater than in any of the channels tried by the French engineers. It

was necessary therefore in adopting the plan of arranging the

different channels in classes of approximately similar roughness to

increase the number of classes. Especially an additional class was

required for channels obstructed by detritus.

Encyclopaedia Britannica, 11th Edition, "Husband" to "Hydrolysis" Volume 14, Slice 1 · 第 122 / 207 题